3.3 Statements of the second law of thermodynamics
As was already stated above, the first law of thermodynamics
characterises quantitatively the processes of conversion of energy.
The second law of thermodynamics characterises the qualitative
side of these processes. The first law provides all that is necessary to
compose the energy balance of a process. However, it gives no indications
whether this or another process is feasible. Meanwhile, by far not all
processes can be practically realized.
It should be stressed that the second law of thermodynamics, as well as
the first, is based on experience.
In the most general form the second law of thermodynamics can be stated
as follows:
Every actual spontaneous process is irreversible.
This sufficiently obvious conclusion was discussed in the preceding section.
All other statements of the second law of thermodynamics are private cases of
the most general statement.
In 1850 R. Clausius proposed the following
statement of the second law of thermodynamics:
Heat cannot pass
spontaneously from a body of lower temperature to a body of
higher temperature.
W. Thomson (Lord Kelvin) in 1851 suggested the following statement:
It is impossible, by means of an inanimate material agency, to derive mechanical
effect from any portion of matter by cooling it below the temperature of the
coldest of the surrounding objects.
M. Planck suggested the following statement:
It is impossible to construct an engine, which, when working in a
complete cycle, will produce no effect other than the
raising of a weight and the cooling of a heat source.
By a machine operating in a cycle is meant an engine converting heat
into work in a cyclic process. Indeed, if it were possible to construct a heat
engine that would simply extract heat from some source and, operating in a
cycle, convert the heat into work, this would violate the previously formulated
statement that a system is capable of performing work only when this system is
out of equilibrium (in particular, as applied to a heat engine, when there is a
difference between the temperatures of the heat source and sink in the system).
If there were no restrictions imposed by the second law of
thermodynamics, this would mean that it is possible to construct a heat engine
with only a heat (high temperature) source. Such an engine could operate at the
expense of cooling, for instance, water in the ocean. This process could
continue until the entire internal energy of the ocean would be converted into
work. A heat engine which would perform in this way was given the name of a perpetual
motion machine of the second kind by Wilhelm Ostwald
(as distinguished from a perpetual motion machine of the first kind, operating
against or violating the law of conservation of energy). In accordance with the
foregoing, the statement of the second law of thermodynamics, suggested by
Planck, can be modified to run as follows;
It is impossible to build a perpetual motion machine of the second kind.
It should be noted that the existence of a perpetual motion machine of
the second kind does not violate the first law of thermodynamics; in fact, in
this engine work would not be created from nothing, but at the expense of the
internal energy of a heat source.
An important feature of heat processes should be emphasized. Mechanical
work, electrical work, the work of magnetic forces, etc. can be fully converted
into heat. But, as regards heat, only a fraction of it can be converted in a
cyclic process into mechanical and other kinds of work; the other fraction of
heat must inevitably be transferred to a low-temperature heat source (or sink).